1. Electrical resistivity and thermodynamic properties of the ferromagnet Nd2Pt2In
- Author
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Dariusz Kaczorowski, André M. Strydom, J.J. Mboukam, M.B. Tchoula Tchokonté, B.M. Sondezi, A.K.H. Bashir, and K. Ramesh Kumar
- Subjects
Physics ,Phase transition ,Magnetic moment ,Condensed matter physics ,Mechanical Engineering ,Metals and Alloys ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Heat capacity ,Magnetic susceptibility ,symbols.namesake ,Magnetization ,Mechanics of Materials ,Electrical resistivity and conductivity ,0103 physical sciences ,Materials Chemistry ,symbols ,Magnetic refrigeration ,Einstein solid ,010306 general physics ,0210 nano-technology - Abstract
The Nd 2 Pt 2 In compound was investigated by means of electrical resistivity ρ ( T ) , heat capacity C p ( T ) , magnetic susceptibility χ ( T ) , magnetization M ( μ 0 H ) and magnetocaloric effect (MCE) measurements. The material orders ferromagnetically at T C = 16 K with a second - order phase transition. In the ordered state, ρ ( T ) can be represented in terms of ferromagnetic (FM) spin - wave dispersion with an energy gap Δ R = 13(1) K in zero field. In concert, the C p ( T ) data in this region can be well described by the same model getting Δ C = 8(1) K in zero field. Above T C , the ρ ( T ) variation is characteristic of electron - phonon interaction in the presence of s − d scattering and crystalline-electric field (CEF). The 4 f - electron specific heat shows a Schottky - type anomaly around 60 K associated with CEF. On the other hand, C p ( T ) data of the non-magnetic homologue La 2 Pt 2 In can be described by the Debye - Einstein model, giving a Debye and Einstein temperature values of 190.3(5) K and 69.8(7) K respectively. At high temperatures, the χ ( T ) data follows the Curie - Weiss relation with an effective magnetic moment μ e f f = 3.61(2) μ B and a Weiss temperature θ p = 17(1) K. The magnitude of MCE was estimated from the isothermal magnetization data to be 6.25 J/(kg.K), 5.01 J/(kg.K), 3.18 J/(kg.K) and 0.47 J/(kg.K) for a field change of 7 T, 5 T, 3 T and 1 T, respectively. The characteristic behaviour of the isothermal magnetic entropy change points to a second - order character of the FM phase transition.
- Published
- 2018
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